示例#1
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    def plot_coordinates(self, ts, qs, fig=None, ax=None, labels=None):
        fig, ax = default_fig(fig, ax)

        ax.set_title('Coordinates', fontsize=16)
        ax.set_xlabel('$\\theta_1$ (rad)', fontsize=16)
        ax.set_ylabel('$\\theta_2$ (rad)', fontsize=16)
        ax.plot(*qs.T, linewidth=3)

        return fig, ax
    def plot_states(self, ts, xs, fig=None, ax=None, labels=None):
        fig, ax = default_fig(fig, ax)

        ax.set_title('States', fontsize=16)
        ax.set_xlabel('$\\theta$ (rad)', fontsize=16)
        ax.set_ylabel('$\\dot{\\theta}$ (rad / sec)', fontsize=16)
        ax.plot(*xs.T, linewidth=3)

        return fig, ax
示例#3
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    def plot_tangents(self, ts, xs, fig=None, ax=None, skip=1):
        fig, ax = default_fig(fig, ax)

        ax.set_title('Tangent Vectors', fontsize=16)
        ax.set_xlabel('$\\theta_1$ (rad)', fontsize=16)
        ax.set_ylabel('$\\theta_2$ (rad)', fontsize=16)
        ax.plot(*xs[:, :2].T, linewidth=3)
        ax.quiver(*xs[::skip, :2].T, *xs[::skip, 2:].T, angles='xy')

        return fig, ax
示例#4
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    def plot_states(self, ts, xs, fig=None, ax=None, labels=None):
        fig, ax = default_fig(fig, ax)

        ax.set_title('States', fontsize=16)
        ax.set_xlabel('$\\theta$ (rad)', fontsize=16)
        ax.set_ylabel('$\\dot{\\theta}$ (rad / sec)', fontsize=16)
        ax.plot(xs[:, 0], xs[:, 2], linewidth=3, label='$\\theta_1$')
        ax.plot(xs[:, 1], xs[:, 3], linewidth=3, label='$\\theta_2$')
        ax.legend(fontsize=16)

        return fig, ax
示例#5
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    def plot_actions(self, ts, us, fig=None, ax=None, labels=None):
        fig, ax = default_fig(fig, ax)

        if labels is None:
            labels = ['$\\tau_1$ (N $\\cdot m$)', '$\\tau_2$ (N $\\cdot$ m)']

        ax.set_title('Actions', fontsize=16)
        ax.set_xlabel(labels[0], fontsize=16)
        ax.set_ylabel(labels[1], fontsize=16)
        ax.plot(*us.T, linewidth=3)

        return fig, ax
示例#6
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    def plot_physical(self, ts, xs, fig=None, ax=None, skip=1):
        fig, ax = default_fig(fig, ax)

        xs, zs, thetas = xs[:, :3].T
        dirs = array([sin(thetas), cos(thetas)])[:, ::skip]

        ax.set_title('Physical Space', fontsize=16)
        ax.set_xlabel('$x$ (m)', fontsize=16)
        ax.set_ylabel('$z$ (m)', fontsize=16)
        ax.quiver(xs[::skip], zs[::skip], *dirs, angles='xy')
        ax.plot(xs, zs, linewidth=3)
        ax.axis('equal')

        return fig, ax
    def plot_physical(self, ts, xs, fig=None, ax=None, skip=1):
        fig, ax = default_fig(fig, ax)

        _, l, g = self.params
        thetas = xs[:, 0]
        rs = l * array([sin(thetas), cos(thetas)])
        zs = 0 * thetas[::skip]

        ax.set_title('Physical space', fontsize=16)
        ax.set_xlabel('$x$ (m)', fontsize=16)
        ax.set_ylabel('$z$ (m)', fontsize=16)
        ax.plot([zs, rs[0, ::skip]], [zs, rs[1, ::skip]], 'k')
        ax.plot(*rs, linewidth=3)
        ax.axis('equal')

        return fig, ax
示例#8
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    def plot_physical(self, ts, xs, fig=None, ax=None, skip=1):
        fig, ax = default_fig(fig, ax)

        _, _, l_1, l_2, _ = self.params
        theta_1s, theta_2s = xs[:, :2].T
        r_1s = l_1 * array([sin(theta_1s), cos(theta_1s)])
        r_2s = r_1s + l_2 * array(
            [sin(theta_1s + theta_2s),
             cos(theta_1s + theta_2s)])
        zs = 0 * theta_1s[::skip]

        ax.set_title('Physical space', fontsize=16)
        ax.set_xlabel('$x$ (m)', fontsize=16)
        ax.set_ylabel('$z$ (m)', fontsize=16)
        ax.plot([zs, r_1s[0, ::skip]], [zs, r_1s[1, ::skip]], 'k')
        ax.plot([r_1s[0, ::skip], r_2s[0, ::skip]],
                [r_1s[1, ::skip], r_2s[1, ::skip]], 'k')
        ax.plot(*r_1s, linewidth=3)
        ax.plot(*r_2s, linewidth=3)
        ax.axis('equal')

        return fig, ax